All-optical single-atom photon router controlled by a single photon

Abstract

A switch activated by a single control photon for routing a single target photon from either of two switch inputs to either of two switch outputs. The device is based on a single quantum emitter, such as an atom, coupled to a fiber-coupled, chip-based optical micro-resonator. A single reflected control photon toggles the switch from high reflection to high transmission mode, with no additional control fields required. The control and target photons are both in-fiber and practically identical, for compatibility with scalable architectures for quantum information processing.

Claims

1. A device for storing and reading a circular polarization of a photon and for routing a single target photon by a single control photon, the device comprising: a waveguide supporting a first electromagnetic mode and a second electromagnetic mode, wherein the first electromagnetic mode is distinct from the second electromagnetic mode, the waveguide coupled to: a first input port for a photon; a second input port for a photon; a first output port for a photon; and a second output port for a photon; wherein the first input port is distinct from the second input port and the first output port is distinct from the second output port: a quantum emitter having: a first ground state; a second ground state; an excited state; a first transition, between the first ground state and the excited state, the first transition having a first circular polarization; and a second transition, between the second ground state and the excited state, the second transition having a second circular polarization; wherein: the first ground state is distinct from the second ground state; the first circular polarization is opposite of the second circular polarization; the first electromagnetic mode couples to the first transition; and the second electromagnetic mode couples to the second transition.

2. The device of claim 1, wherein the waveguide couples to the quantum emitter via a resonant cavity.

3. The device of claim 2, wherein the resonant cavity is a micro-resonator.

4. The device of claim 1, wherein the waveguide is an optical waveguide.

5. The device of claim 1, wherein the waveguide is a microwave waveguide.

6. The device of claim 1, wherein the quantum emitter is a Rubidium atom.

7. The device of claim 6, wherein the Rubidium atom is a .sup.87Rb atom.

8. The device of claim 1, wherein the micro-resonator is in a transverse magnetic (TM) mode.

9. The device of claim 2, wherein the micro-resonator is a microsphere.

10. The device of claim 9, wherein the microsphere is a silica microsphere.

11. The device of claim 3, wherein the micro-resonator is a micro-toroid.

12. The device of claim 11, wherein the micro-toroid is a silica micro-toroid.

13. The device of claim 3, wherein the micro-resonator is a microdisk.

14. The device of claim 3, wherein the micro-resonator is a ring resonator.

15. The device of claim 4, wherein the optical waveguide comprises a tapered nanofiber and the waveguide is coupled to the quantum emitter via a micro-resonator.

16. The device of claim 15, further comprising a piezo positioning device, for aligning the tapered nanofiber with the micro-resonator.

17. The device of claim 15, wherein an input port is coupled to the tapered nanofiber by an optical circulator.

18. The device of claim 17, wherein the optical circulator is further coupled to an output port.

19. The device of claim 18, wherein the input port is isolated from the output port by the optical circulator.

20. The device of claim 1, wherein the quantum emitter is selected from a group consisting of: an atom, a nitrogen vacancy center, a superconducting quibit, and a quantum dot.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

(1) The subject matter disclosed may best be understood by reference to the following detailed description when read with the accompanying drawings in which:

(2) FIG. 1A is an energy-level diagram of transitions in a quantum emitter which reflects a right-propagating photon.

(3) FIG. 1B is an energy-level diagram of transitions in quantum emitter which reflects a left-propagating photon.

(4) FIG. 1C is an energy-level diagram of a quantum emitter which transmits a right-propagating photon with no transitions.

(5) FIG. 1D is an energy-level diagram of quantum emitter which transmits a left-propagating photon with no transitions.

(6) FIG. 2 is a schematic diagram of a photon routing device according to an embodiment of the present invention.

(7) FIG. 3A illustrates a physical configuration of a photon routing device according to an embodiment of the present invention.

(8) FIG. 3B illustrates a physical configuration of a photon routing device according to another embodiment of the present invention.

(9) FIG. 3C illustrates details of the port arrangement for the configuration shown in FIG. 3B.

(10) For simplicity and clarity of illustration, elements shown in the figures are not necessarily drawn to scale, and the dimensions of some elements may be exaggerated relative to other elements. In addition, reference numerals may be repeated among the figures to indicate corresponding or analogous elements.

DETAILED DESCRIPTION

(11) Embodiments of the invention use the above-described mechanism for optical switching, by introducing memory into the system, that is, making the reflection of a single control photon toggle the internal state of the quantum emitter.

(12) Various embodiments of the present invention utilize bi-directional photon paths. For simplicity, the descriptions and illustrations herein arbitrarily refer to the first direction of photon propagation as right (or equivalently left-to-right) and the second direction of photon propagation as left (or equivalently right-to-left). It is understood, however, that this is non-limiting, and that other distinguishing representations can equivalently be used (e.g., up and down, forward and backward, etc.) to describe the same embodiments.

(13) In an embodiment of the present invention, a photon is considered to be circularly polarized if the probability of detecting the photon in a particular state of circular polarization is greater than . In a related embodiment of the invention, the two distinct circular polarization states correspond to two distinct electromagnetic modes of a waveguide. In another related embodiment, the waveguide is an optical waveguide. In a further related embodiment, the waveguide is a microwave waveguide.

(14) In certain embodiments of the invention, the waveguide couples directly to the quantum emitter. In other embodiments, the waveguide couples to the quantum emitter indirectly via a resonant cavity. In a related embodiment, a circular polarization of a photon corresponds to a Transverse Magnetic (TM) mode of a waveguide.

(15) In various embodiments of the invention, the two distinct quantum emitter transitions from the two distinct ground states to the excited state correspond respectively to the two different circular polarizations.

(16) According to an embodiment of the invention, an initial ground state of the quantum emitter is at m.sub.F=1 with an incoming .sup.+ probe photon. Destructive interference between the probe and the .sup.+ photon emitted by the quantum emitter forces the quantum emitter to emit a .sup. photon in the opposite direction, thereby deterministically ending at a final ground state at m.sub.F=+1. As a result, any subsequent .sup.+ photons will not interact with the quantum emitter and will accordingly be transmitted. Symmetrically, at this stage the system becomes reflective to .sup. photons coming right-to-left from the right.

(17) FIG. 1A conceptually illustrates the above embodiment, implemented by a configuration for a three-level quantum emitter 101 which has a transition 103 from a first ground state 113 (m.sub.F=1) to an excited state 115; and a transition 105 from excited state 115 to a second ground state 117 (m.sub.F=+1). Transition 103 is coupled only to an input photon having a left-to-right direction of propagation, shown for a .sup.+ input photon 111. Transition 105 is coupled only to an output photon having a right-to-left direction of propagation, shown for a .sup. output photon 109. As discussed previously, left-to-right propagating output photon 107 is 180 degrees out of phase with input photon 111, and through destructive interference, the net transmission 119 is zero.

(18) FIG. 1B conceptually illustrates the symmetrical complement of the arrangement in FIG. 1A, in which three-level quantum emitter 101 has a transition 123 from second ground state 117 (m.sub.F=+1) to excited state 115; and a transition 125 from excited state 115 to first ground state 113 (m.sub.F=1). Transition 123 is coupled only to an input photon having a right-to-left direction of propagation, shown for a .sup. input photon 131. Transition 125 is coupled only to an output photon having a left-to-right direction of propagation, shown for a .sup.+ output photon 129. As discussed previously, right-to-left propagating output photon 127 is 180 degrees out of phase with input photon 131, and through destructive interference, the net transmission 139 is zero.

(19) FIG. 1C conceptually illustrates the above embodiment in the case when three-level quantum emitter 101 is in second ground state 117 for a right-propagating .sup.+ input photon 151. No transition occurs in this case: three-level atom 101 remains in second ground state 117 and .sup.+ photon 151 is transmitted without reflection.

(20) FIG. 1D conceptually illustrates the above embodiment in the case when three-level quantum emitter 101 is in first ground state 113 for a left-propagating .sup. input photon 171. No transition occurs in this case: three-level atom 101 remains in first ground state 114 and .sup. photon 171 is transmitted without reflection.

(21) For certain embodiments of the present invention, an input photon may serve the purpose of setting or discovering the state of the quantum emitter. In a non-limiting example, the input photon may be intended to put the quantum emitter into a selected state (to reflect or transmit a photon); in this case, such an input photon may be denoted as a control photon, and a subsequent input photon which is to be routed by the quantum emitter (i.e., switched to a selective path via reflection or transmission by the quantum emitter) may be denoted as a target photon. In another non-limiting example, the input photon may be intended to discover the quantum emitter's state; in this case, such an input photon may be denoted as a probe photon. Structurally, however, there is no qualitative difference between a control photon, a target photon, and a probe photon. These terms are used in the context of particular embodiments simply according to the intended purpose of the photon.

(22) FIG. 2 schematically illustrates an embodiment of the present invention, which provides a symmetric toggle-switch 200 with two inputs (an input 201 and an input 203), two outputs (an output 205 and an output 207), and two internal states (state 113 and state 117), where a transition of atom 101 (transition 105 or transition 125) toggles the state of switch 200 (accompanied by a reflection of an input control photon) for routing one or more subsequent target photons. A first input 201 and a second input 203 accept photons for control of the switch and/or routing of photons by switch 200. Photon routing is according to the state of switch 200, in keeping with the transition rules shown in FIG. 1A through FIG. 1D: when three-level quantum emitter 101 is in state 113, a photon input into input port 1 201 undergoes a reflection 211 to output port 1 205;

(23) when three-level quantum emitter 101 is in state 117, a photon input into input port 1 201 continues with a transmission 221 to output port 2 207; when three-level quantum emitter 101 is in state 117, a photon input into input port 2 203 undergoes a reflection 213 to output port 2 207; and when three-level quantum emitter 101 is in state 113, a photon input into input port 2 203 continues with a transmission 223 to output port 1 205. In a related embodiment, a conventional time-bin protocol is used to define a first input photon as the control photon, and a second input photon as the target, to be routed from a selected input to a selected output.

(24) FIG. 3A illustrates a physical configuration of an embodiment of the present invention, in which three-level quantum emitter 101 is a single Rubidium atom. In a related embodiment, the Rubidium atom is the isotope .sup.87Rb. In another related embodiment, three-level atom 101 is coupled to a chip-based whispering-gallery mode (WGM) silica microsphere resonator 301. Light is evanescently coupled to and from resonator 301 by a tapered nanofiber 303. The coupling .sub.ex between resonator 301 and nanofiber is 303 set by careful alignment of their relative position using a piezo positioning system 371. In other embodiments of the present invention, micro-resonator 301 is a microdisk resonator; in additional embodiments, micro-resonator 301 is a micro-toroid resonator; in still further embodiments, micro-resonator 301 is a ring resonator.

(25) In various embodiments of the invention, a transverse-magnetic (TM) mode of the micro-resonator is used, which approximates to a high degree the coupling of .sup.+ and .sup. polarizations to opposite directions of propagation. It is known that the polarization in the evanescent wave region is very close to .sup.+ in one direction, and .sup. in the other, with minimal cross-contamination. In these embodiments the polarizations of the respective .sup.+ and .sup. input photons are the polarizations that maximally couple to the CW and CCW modes of the cavity resonance. Thus, there is a one-to-one correspondence between the direction in which the photon propagates in the fiber, and the transition in the atom. A .sup.+ photon input in a pulse 311 propagating in a left-to-right direction 313 from a face 305 of nanofiber 303 triggers a transition from the m.sub.F=1 state to the m.sub.F=+1 state (and the input photon is reflected), whereas a .sup. input photon in a pulse 315 propagating in a right-to-left direction 317 from a face 307 of nanofiber 303 triggers a transition from the m.sub.F=+1 state to the m.sub.F=1 state (and the input photon in pulse 315 is reflected in a left-to-right direction 325).

(26) A photon automatically has the proper polarization to initiate the transition if it is sent from the proper input port and is resonantly coupled to the cavity. As described and illustrated herein, if the atom is already in the m.sub.F=+1 state, left-to-right .sup.+ input photon in pulse 311 triggers no transition (and input photon in pulse 311 is transmitted in a direction 325 without reflection); if the atom is already in the m.sub.F=1 state, right-to-left .sup. input photon in pulse 315 triggers no transition (and the input photon in pulse 315 is transmitted in a direction 323 without reflection).

(27) According to an embodiment of the present invention, resonator 301 and the probe photon are tuned to be resonant with the F=1.fwdarw.F=0 transition of the .sup.87Rb D.sub.2 line. As atoms in the state m.sub.F=0 barely interact with the TM mode, by choosing this manifold the desired -configuration is attained, as illustrated in FIG. 1A and FIG. 1B, although, for this specific non-limiting case, at the price of decreasing the coherent coupling rate g by a factor of the square root of 3 compared to the cycling transition (F=2.fwdarw.F=3), in which mean g=27 MHz is measured. To reach the fast cavity limit .sub.ex is set to 30 MHz, corresponding to mean g.sup.2/=2.2.

(28) FIG. 3B illustrates a physical configuration of another embodiment of the present invention, in which input ports are separated and isolated from output ports, meaning that only input photons propagate in input fibers, and only output photons propagate in output fibers. A first input fiber 321 is coupled to tapered nanofiber 303 by an optical circulator 351. In addition, a first output fiber 325 is also coupled to tapered nanofiber 303 by optical circulator 351. Likewise, a second input fiber 323 is coupled to tapered nanofiber 303 by an optical circulator 353, and a second output fiber 327 is also coupled to tapered nanofiber 303 by optical circulator 353.

(29) Although photon propagation in tapered nanofiber 303 is bidirectional, optical circulator 351 enables uni-directional photon propagation in input fiber 321 (in which .sup.+ photons propagate in direction 313) and in output fiber 325 (in which .sup. photons propagate in a direction 381). Likewise, optical circulator 353 enables uni-directional photon propagation in input fiber 323 (in which .sup. photons propagate in direction 317) and in output fiber 327 (in which .sup.+ photons propagate in a direction 383).

(30) FIG. 3C illustrates details of the configuration of FIG. 3B, to show how optical circulator 351 and optical circulator 353 separate and isolate inputs from outputs. In this embodiment, first input port 201 is the face of optical fiber 321, and first output port 205 is the face of optical fiber 325. Photons (.sup.+) in input fiber 321 propagating into optical circulator 351 via a circulator port 341 are routed from a circulator port 343 into tapered nanofiber 303. However, photons (.sup.) propagating from nanofiber 303 into optical circulator 351 via circulator port 343 are routed by a circulator port 345 into output fiber 325. Likewise, second input port 203 is the face of optical fiber 323, and second output port 207 is the face of optical fiber 327. Photons (.sup.) in input fiber 323 propagating into optical circulator 353 via a circulator port 361 are routed from a circulator port 363 into tapered nanofiber 303. However, photons (.sup.+) propagating from nanofiber 303 into optical circulator 353 via circulator port 363 are routed by a circulator port 365 into output fiber 327.

NON-LIMITING EXAMPLE OF DETECTING PRESENCE AND STATE OF A QUANTUM EMITTER

(31) The presence of a single atom within the evanescent wave of the TM mode can be identified by sending weak (averaging about 2.5 photons per pulse) and short (approximately 15 ns FWHM) pulses in the nanofiber in alternating directions and detecting at least three reflected photons within less than 400 ns. Interleaved between the detection pulses are much weaker pulses (an average of 0.24 photons in each pulse) and longer (approximately 50 ns FWHM) target pulses, whose purpose is to accurately measure single-photon reflection and transmission properties of the switch-router. The last detection pulse before each target pulse serves as the control to set the atom in a predetermined initial state. The pulse sequence includes control pulses in both directions, thereby preparing the atom half of the time in m.sub.F=1, and half of the time in m.sub.F=+1, with the target pulse always polarized .sup.+.

OTHER USES

(32) Besides serving as a switch or router for photons, an embodiment of the present invention can also serve as device for storing a classical bit of information, encoded in the state of the quantum emitter. In another embodiment, a qubit (quantum bit) of information can be stored, wherein the qubit is in a superposition of two distinct states.